Lecture 18. MSMPR Crystallization Model

Similar documents
MATH Midterm Examination Victor Matveev October 26, 2016

D.S.G. POLLOCK: TOPICS IN TIME-SERIES ANALYSIS STATISTICAL FOURIER ANALYSIS

x 2 x 3 x b 0, then a, b, c log x 1 log z log x log y 1 logb log a dy 4. dx As tangent is perpendicular to the x axis, slope

F O R SOCI AL WORK RESE ARCH

WEST VIRGINIA UNIVERSITY

The Excel FFT Function v1.1 P. T. Debevec February 12, The discrete Fourier transform may be used to identify periodic structures in time ht.

Axial Temperature Distribution in W-Tailored Optical Fibers

[1 & α(t & T 1. ' ρ 1

, the random variable. and a sample size over the y-values 0:1:10.

Electrostatics. . where,.(1.1) Maxwell Eqn. Total Charge. Two point charges r 12 distance apart in space

Unit -2 THEORY OF DILUTE SOLUTIONS

Examination No. 3 - Tuesday, Nov. 15

are specified , are linearly independent Otherwise, they are linearly dependent, and one is expressed by a linear combination of the others

Framework for functional tree simulation applied to 'golden delicious' apple trees

The generalized marginal rate of substitution

Markov processes and the Kolmogorov equations

Quantum Mechanics for Scientists and Engineers. David Miller

probability of k samples out of J fall in R.

Characterization of R-134a Superheated Droplet Detector for Neutron Detection

Physical Chemistry Laboratory I CHEM 445 Experiment 2 Partial Molar Volume (Revised, 01/13/03)

Analysis of pressure wave dynamics in fuel rail system

Fourier Method for Solving Transportation. Problems with Mixed Constraints

Solutions. Definitions pertaining to solutions

K [f(t)] 2 [ (st) /2 K A GENERALIZED MEIJER TRANSFORMATION. Ku(z) ()x) t -)-I e. K(z) r( + ) () (t 2 I) -1/2 e -zt dt, G. L. N. RAO L.

Hº = -690 kj/mol for ionization of n-propylene Hº = -757 kj/mol for ionization of isopropylene

Chapter 3.1: Polynomial Functions

Lecture 21: Signal Subspaces and Sparsity

5.1 Two-Step Conditional Density Estimator

Study of Energy Eigenvalues of Three Dimensional. Quantum Wires with Variable Cross Section

Motor Stability. Plateau and Mesa Burning

MATH 6101 Fall 2008 Series and a Famous Unsolved Problem

Mean residual life of coherent systems consisting of multiple types of dependent components

Differentiating Functions & Expressions - Edexcel Past Exam Questions


ETIKA V PROFESII PSYCHOLÓGA

Claude Elysée Lobry Université de Nice, Faculté des Sciences, parc Valrose, NICE, France.

Limits and Continuity. 2 lim. x x x 3. lim x. lim. sinq. 5. Find the horizontal asymptote (s) of. Summer Packet AP Calculus BC Page 4

Chapter 4. Problem Solutions

Q Scheme Marks AOs. Notes. Ignore any extra columns with 0 probability. Otherwise 1 for each. If 4, 5 or 6 missing B0B0.

The Acoustical Physics of a Standing Wave Tube

MATH 6101 Fall Problems. Problems 11/9/2008. Series and a Famous Unsolved Problem (2-1)(2 + 1) ( 4) 12-Nov-2008 MATH

ALE 26. Equilibria for Cell Reactions. What happens to the cell potential as the reaction proceeds over time?

Probability Refresher and Cycle Analysis. Spring 2018 CS 438 Staff, University of Illinois 1

Sound Absorption Characteristics of Membrane- Based Sound Absorbers

Coupled Inductors and Transformers

4F-5 : Performance of an Ideal Gas Cycle 10 pts

A Study on Estimation of Lifetime Distribution with Covariates Under Misspecification

BIO752: Advanced Methods in Biostatistics, II TERM 2, 2010 T. A. Louis. BIO 752: MIDTERM EXAMINATION: ANSWERS 30 November 2010

MATH 174: Numerical Analysis I. Math Division, IMSP, UPLB 1 st Sem AY

DEPARTMENT OF ELECTRICAL ENGINEERING DIT UNIVERSITY HIGH VOLTAGE ENGINEERING

On the structure of space-time and matter as obtained from the Planck scale by period doubling in three and four dimensions

IE 400 Principles of Engineering Management. Graphical Solution of 2-variable LP Problems

Conventional propellers in CRP-POD configuration. Tests and extrapolation.

5.80 Small-Molecule Spectroscopy and Dynamics

Rates and Mechanisms of Chemical Reactions

UNIQUE FJORDS AND THE ROYAL CAPITALS UNIQUE FJORDS & THE NORTH CAPE & UNIQUE NORTHERN CAPITALS

Multi-objective Programming Approach for. Fuzzy Linear Programming Problems

Chapter 10 Conics, Parametric Equations, and Polar Coordinates Conics and Calculus

A New Method for Finding an Optimal Solution. of Fully Interval Integer Transportation Problems

LA PRISE DE CALAIS. çoys, çoys, har - dis. çoys, dis. tons, mantz, tons, Gas. c est. à ce. C est à ce. coup, c est à ce

Automatic Control III (Reglerteknik III) fall Nonlinear systems, Part 3

f x x c x c x c... x c...

A Hartree-Fock Calculation of the Water Molecule

Grade 3 Mathematics Course Syllabus Prince George s County Public Schools

Modeling of Plasmas and Neutrals Including Plasma-Wall Interaction for Long Term Tokamak Operation

This section is optional.

Modeling and Simulation of Ethylene Polymerization in Industrial Slurry Reactor Series

MATH140 Exam 2 - Sample Test 1 Detailed Solutions

An Investigation of Stratified Jackknife Estimators Using Simulated Establishment Data Under an Unequal Probability Sample Design

2C09 Design for seismic and climate changes

E o and the equilibrium constant, K

Characteristics of helical flow in slim holes and calculation of hydraulics for ultra-deep wells

Chapter 5. Root Locus Techniques

CHAPTER 3 Describing Relationships

PHYSICS. Suppose slit width s are equal, so they produces waves of equal intensity say I. Resultant intensity at any point

Short notes for Heat transfer

Compact Models for Giga-Scale Memory System. Mansun Chan, Dept. of ECE, HKUST

Continuous-time Fourier Methods

Preliminary Test Single Stage Shrinkage Estimator for the Scale Parameter of Gamma Distribution

Sequences, Mathematical Induction, and Recursion. CSE 2353 Discrete Computational Structures Spring 2018

NOTES ON DISTRIBUTIONS

T i t l e o f t h e w o r k : L a M a r e a Y o k o h a m a. A r t i s t : M a r i a n o P e n s o t t i ( P l a y w r i g h t, D i r e c t o r )

Optimum Sizing of a PV-Battery-Diesel Hybrid System for Remote Consumers

Journal of Hazardous Materials

MATH 6101 Fall 2008 Newton and Differential Equations

ChE 471: LECTURE 4 Fall 2003

7 Algebra. 7.1 Manipulation of rational expressions. 5x x x x 2 y x xy y. x +1. 2xy. 13x

P E R E N C O - C H R I S T M A S P A R T Y

CHAPTER 6 : LITERATURE REVIEW

Topic 5 [434 marks] (i) Find the range of values of n for which. (ii) Write down the value of x dx in terms of n, when it does exist.

Machine Learning: Logistic Regression. Lecture 04

Unifying the Derivations for. the Akaike and Corrected Akaike. Information Criteria. from Statistics & Probability Letters,

QUESTIONS ON QUARKONIUM PRODUCTION IN NUCLEAR COLLISIONS

MODIFIED LEAKY DELAYED LMS ALGORITHM FOR IMPERFECT ESTIMATE SYSTEM DELAY

Lecture 10, Principal Component Analysis

Study in Cylindrical Coordinates of the Heat Transfer Through a Tow Material-Thermal Impedance


ERT 318 UNIT OPERATIONS

Assume that the water in the nozzle is accelerated at a rate such that the frictional effect can be neglected.

Krzepnięcie Metali i Stopów, 18 PL ISSN

Transcription:

ecture 18. MSMPR Crystalliati Mdel MSMPR Crystalliati Mdel Crystal-Ppulati alace - Number f crystals - Cumulative umber f crystals - Predmiat crystal sie - Grwth rate

MSMPR Crystalliati Mdel Mixed-suspesi, mixed-prduct-remval (MSMPR) mdel is useful fr the desig ad aalysis f draft-tube, baffled crystallier Assumptis (1) Ctiuus, steay-flw, steay-state perati (2) Perfect mixig f the magma () N classificati f crystals (4) Uifrm degree f supersaturati fr the magma (5) Crystal grwth rate idepedet f crystal sie (6) N crystals i the feed, but seeds are added iitially (7) N crystal breakage (8) Uifrm temperature (9) Mther liqur i prduct magma i equilibrium with the crystals (1) Nucleati rate is cstat, uifrm, ad due t secdary ucleati by crystal ctact (11) Crystal-sie distributi is uifrm i the crystallier ad equal t that i the magma (12) All crystals have the same shape

Crystal-Ppulati alace (1) The crystal-sie distributi ca be estimated as a fucti f the rpm f the draft-tube prpeller ad exteral circulati rate by a crystal-ppulati balace i the MSMPR mdel The umber f crystals per uit sie per uit vlume d( N V ) d Fr a cstat, crystal-sie grwth rate idepedet f crystal sie G d dt 1 V dn d : characteristic crystal sie (e.g. frm a scree aalysis) N : cumulative umber f crystals f sie ad smaller i the magma i the crystallier V : vlume f the mther liqur i the crystallier magma D GDt Gt D law f McCabe t : residece time i the magma i the crystallier fr crystals f sie

Crystal-Ppulati alace (2) Number f crystals i the sie rage d dn Vd Frm the perfect-mixig assumpti fr the magma, umber f crystals withdraw mther - liqur vlume withdraw umber f crystals i crystallier mther - liqur vlume i crystallier umber f crystals withdraw umber f crystals i crystallier mther - liqur vlume withdraw mther - liqur vlume i crystallier Dd D Q D t Q - - : vlumetric flw rate f mther liqur d V i the withdraw prduct magma

Crystal-Ppulati alace () D GDt D Q D t - V ü ý þ - D Q D d Q - GV d GV Takig the limit Reteti time f mther liqur i the crystallier, t V Q d - d Gt Itegrati exp( - G t ) Number f crystals per uit vlume f mther liqur belw sie N V ò d Number f crystals per uit vlume f mther liqur N V T ò d

Crystal-Ppulati alace (4) Cumulative umber f crystals f sie smaller tha, as a fucti f the ttal x ò ò - Gt e d 1 - exp( - Gt ) - Gt e d 1 - e - (/Gt) : dimesiless crystal sie Cumulative distributi (cumulative crystal ppulati) Differetial distributi dx d e - Fr a give value f, x is the fracti f crystals havig a smaller -value

Crystal-Ppulati alace (5) Mmet equati fr a relati f ( ) x ò k d k k ò d k : rder f the mmet Mmet Distributi basis Cumulative Differetial Zerth First Secd Third Number Sie r legth Area Vlume r mass x 1 - e - x 1- ( 1+ ) e - 2 x 1 - ( 1 + + ) e - a 2 x 1 - ( 1 + + + ) e - m 2 2 6 dx d e - dx d e - 2 dx d e - a dx d e - Predmiat crystal sie, pd i terms f the mass distributi: crrespdig t the peak f the differetial-mass distributi æ dx d m ö ç d 2 - - è ø e e - \ pd Gt d 6 6 Gt m 2 6

Crystal-Ppulati alace (6) Grwth rate (G) depeds the supersaturati ad degree f agitati, ad residece time (t) depeds crystallier desig ad perati 1 dn 1 dn æ d ö ç V dt V d è dt ø 1 lim V 1 lim V dn dt d G dt dn d ü ï ý ï ï þ G exp( - G t ) Pwer-law fucti fr the effect f peratig cditis k G M N i j r N T exp( - G G t ) This equati ca be used t btai ucleati ad grwth rates

Crystal-Ppulati alace (7) Number f crystals per uit vlume f mther liqur c NT V Mass f crystals per uit vlume f mther liqur m c ò m d m p : mass f a particle, m p fv r p m 6 f r ( Gt ) p c v p 4 Number f crystals per uit mass f crystals c 1 m 6 f r ( Gt ) c v p Nucleati rate C ò d tg e d tg 9 G t 2 f r v p pd 9C ò - c mcv 2 f r C : mass rate f prducti f crystals v p V pd pd f v : vlume shape factr defied by v f D p v p i